Thermal analysis instrument

Abstract: The temperature of a heat reservoir (1) is varied according to a linear function which is AC modulated. At this time, the temperature difference between two points (9, 11) located in a heat flow path going from the heat reservoir to an unknown sample (8) is measured. Also, the temperature difference between two points (10, 12) located in a heat flow path going from the heat reservoir to a reference sample (7) is measured. These two pairs of points are arranged symmetrically. Then, the resulting signals are demodulated, and each signal is divided into an AC component and a low-frequency component. Using these signals, the DSC signal is separated into a heat capacity component and a latent heat component.

Description: The present invention relates to a thermal analysis instrument which receives a signal indicating changes in a physical or chemical property of an unknown sample and measures the signal as a function of the unknown sample with respect to temperature or time. In particular, the present invention relates to, but not exclusively to a differential scanning calorimeter (DSC) in which the aforementioned measured signal takes the form of a differential thermal flow between the unknown sample and a reference sample. U.S. Patent No. 5,224,775 discloses a method and apparatus for separating a signal obtained from a heat flux DSC into a reversible component and an irreversible component by subjecting linear temperature control of an unknown sample to AC modulation. While ordinary DSC instruments control the temperature of an unknown sample linearly, the present invention is directed especially to divide a DSC signal into a component reflecting a reversible phenomenon and a component reflecting an irreversible phenomenon. For this purpose, the sample temperature is AC modulated, and the obtained signal is demodulated and analysed. On the other hand, an AC calorimeter measures minute temperature variations of an unknown sample when minute thermal vibrations are given to the unknown sample, and determines the heat capacity of the unknown sample according to the ratio between the amplitude of the quantity of heat acting as a stimulus and the amplitude of the sample temperature acting as a response. With respect to this AC calorimeter, the following papers are known: Hatta et al., "Studies on Phase Transitions by AC Calorimetry," Japanese Journal of Applied Physics, Vol. 20, No. 11, 1981, pp. 1995-2011; and Dixon et al., "A differential AC Calorimeter for Biophysical Studies," Analytical Biochemistry, Vol. 121, pp. 55-61 . A DSC signal becomes a powerful tool when a physical or chemical change of an unknown sample is analysed in relation to temperature. The DSC signals contain both information about the heat capacity of the unknown sample and information regarding the latent heat. In one method, the specific heat of the unknown sample is found from the DSC signal when no latent heat is present. In another known method, a baseline is drawn empirically to remove the component reflecting the heat capacity of the unknown sample from the DSC signal and thus the latent heat of the unknown sample is correctly found. These and other known methods have enjoyed wide acceptance. However, when the nature of the unknown sample provides complex data about behaviours of the heat capacity and latent heat is interpreted, possibly empirical elements as described above are involved. Therefore, the nature of the unknown sample is frequently misinterpreted. It is considered that the cause of this drawback arises from the fact that when the DSC instrument itself is producing a signal, the instrument does not separate a component associated with heat capacity of the unknown sample from a component associated with the latent heat of the unknown sample. This is one of the problems that the present invention is intended to solve. It is an object of the invention to provide an instrument for automatically separating the heat capacity component of a signal and the latent heat component without relying on a human, which would have been impossible to achieve by the prior art DSC instrument. It is expected that if the instrument automatically performs this separation or discrimination, then the aforementioned human errors in interpretation of signals will decrease greatly. In contrast to this, the signal from the AC calorimeter does not contain any component attributed to the latent heat of the unknown sample. This is discussed in the above cited paper by Hatta et al. which describes a technique in conjunction with figure 14 therein. In particular, results of the DSC are compared with results of the AC calorimeter. A component reflecting the heat capacity of the unknown sample is found from the latter results. A component reflecting the latent heat of the unknown sample is found from the difference between the former results and the latter results. In this case, the same sample is investigated by two kinds of instruments, i.e., the DSC and the AC calorimeter, separately. Then their results must be compared. In this way, cumbersome operations are needed. On the other hand, the instrument disclosed in U.S. Patent No. 5,224,775 is claimed to divide the DSC signal into both a reversible component and an irreversible component. However, one who scrutinises the contents of the embodiment would recognise that the technique used to derive the reversible component very closely resembles the method of determination of the heat capacity in the AC calorimeter. Hence, there is the possibility that this technique becomes a means for solving the above-described problem. However, as disclosed in this patent, the instrument is based on the so-called heat flux DSC structure. In particular, the temperature difference between the unknown sample and the reference sample is transformed into the difference between two heat flows one of which is directed from the unknown sample to a heat reservoir, the other being directed from the reference sample to the heat reservoir. Then, the heat flow difference is measured. In principle, only the temperature difference between the unknown sample and the reference sample is measured. Hence, the AC heat capacity of the unknown sample cannot be found precisely for the following reason. In order to obtain the differential heat capacity between the unknown sample and the reference sample, it is necessary to find the difference between the heat flow amplitude on the side of the unknown sample and the heat flow amplitude on the side of the reference sample. This difference cannot be measured precisely unless these AC heat flows are in phase. In practice, during measurement, if the unknown sample undergoes a transition such as melting, the phase of the AC heat flow on the side of the unknown sample varies greatly. This makes it impossible to precisely measure the AC heat capacity of the unknown sample. The inventors and others of the above-described patent have documented the melting of polyethylene terephthalate which was measured with an instrument based on the description of the aforementioned patent. The melting of microscopic structures inside the unknown sample and recrystallisation were observed, based on the behaviour of the separation of the data into a reversible component and an irreversible component. Nonetheless, in our experiments it has been demonstrated that the behaviour of the separation of the data into the reversible component and the irreversible component varies simply by changing the amount of the reference sample: irrespective of the nature of the unknown sample. Consequently, when measuring using such a system, the signal obtained, based on the above patent, reflects neither the heat capacity of the unknown sample nor the nature itself of the unknown sample. This situation can be easily understood from considerations which will be explained using a diagram as shown in Fig. 2. Specially, [Ts] expresses a vector indicating the AC temperature of an unknown sample. [Tr] expresses a vector indicating the AC temperature of a reference sample. Square brackets, [ ], are used to indicate vectors. dT = [Ts] - [Tr] . A temperature differenence signal, is an archetype of the DSC signal from a heat flux DSC. Generally, if [Ts] and [Tr] differ in sense, we have the relationship | [Ts] - [Tr] | ≠ | [Ts] | - | [Tr] | This can also be understood from the fact that the difference between the lengths of two sides of the triangle is different from the length of the other one side. In summary, the instrument disclosed in U.S. Patent No. 5,224,775 is also unsuccessful in extracting the heat capacity component of the DSC signal by the instrument itself. To solve the above problems, the present invention uses the structure of a conduction type calorimeter. In particular, the heat flow between an unknown sample and a heat reservoir is found from the temperature difference between two points along a heat flow path going from the heat reservoir to the unknown sample. Independently of this, the heat flow between a reference sample and the heat reservoir is found from the temperature difference between two points along a heat flow path going from the heat reservoir to the reference sample. The temperature of the heat reservoir is controlled by a ramp function which is modulated by an AC function, in the same way as in U.S. Patent No. 5,224,775. A heat flow signal on the side of the unknown sample and a heat flow signal on the side of the reference sample are independently demodulated and their respective heat flow amplitudes are found. Then, the difference between them is taken to obtain the amplitude of an excessive heat flow supplied to the unknown sample. This excessive heat flow amplitude is divided by a sample temperature amplitude and an AC angular frequency which are found independently of the excessive heat flow amplitude. Thus, the excessive heat capacity of the unknown sample with respect to the reference sample is obtained, in the same manner as in an AC calorimeter. Furthermore, the excessive heat capacity of the unknown sample is multiplied by the average temperature change rate of the unknown sample so that the excessive heat capacity may be transformed into the dimension of heat flow. This is produced as a heat capacity component signal. Although a DSC signal contains both information concerning the heat capacity of an unknown sample and information concerning the heat capacity, the heat capacity component signal reflects only the former component and represents the baseline of the DSC signal. The heat flow on the side of the unknown sample is passed through a low-pass filter. The heat flow on the side of the reference sample is processed similarly to derive a low-frequency signal. This low frequency signal is subtracted from the low-frequency signal from the aforementioned low-pass filter. As a result, a kinetic component signal containing information regarding the latent heat of the unknown sample is obtained. The structure described above operates in such a way that the instrument itself separates and extracts information concerning the heat capacity of the unknown sample and information concerning the latent heat. The former information has conventionally been included inevitably in the DSC signal. The latent heat is produced when the unknown sample causes a transition or reaction. The resulting heat capacity component signal indicates the position of the correct baseline about the original DSC data. Since the kinetic component signal does not change when the heat capacity of the unknown sample changes, information about an enthalpy produced during a transition or reaction can be known precisely. Embodiments of the present invention will now be described with reference to the accompanying drawings, of which: Figure 1 is a diagram illustrating one example of the invention; and Figure 2 is a diagram illustrating the prior art temperature vectors. One embodiment of the present invention is described in detail below by referring to figure 1. In figure 1, a heat reservoir 1 of substantially H-shaped cross-section is made of silver. The temperature (Th) of the heat reservoir 1 is measured by a furnace temperature-measuring thermocouple 2. The signal from the thermocouple is fed to a furnace temperature control circuit 3, which in turn supplies electric power to a heater 4 enclosed in an insulator. In this way, the temperature of the heat reservoir 1 is controlled. For this purpose, a well-known PID (proportional plus integral plus derivative) action is utilised. In particular, the difference between a temperature based on a desired temperature program delivered from a processor 16 and the output temperature from the furnace temperature-measuring thermocouple 2 is produced and subjected to PID operations in the furnace temperature control circuit 3. The output power from the control circuit 3 is supplied to the heater 4. A heat conduction plate 6 made of constantan (copper-nickel alloy) is joined to the centre of the heat reservoir 1 such that the centre of the plate is fixed inside the heat reservoir 1. An unknown sample portion 6a is formed like a platform at one end of the heat conduction plate 6. A reference sample portion 6b is formed at the other end. Thus, these two portions 6a and 6b are arranged symmetrically. An unknown sample 8 loaded in an aluminum container 7 is placed on the unknown sample portion 6a. A hollow container 7 is placed on the reference sample portion 6b. A cover 5 made of silver is mounted at the top of the heat reservoir 1 to permit the containers 7 to be inserted and withdrawn. A chromel-alumel thermocouple 9 (of the K type) comprising a chromel line 9a forming a positive pole and an alumel line 9b forming a negative pole is welded to the underside of the unknown sample portion 6a to measure the temperature of the unknown sample 8. Also, a thermocouple 10 comprising a chromel line 10a forming a positive pole and an alumel line 10b forming a negative pole is welded to the underside of the reference sample portion 6b to secure the symmetry of the unknown sample portion 6a and the reference sample portion 6b. In practice, therefore, the thermocouple 10 measures no temperature. A chromel line 11a is welded to a given point 11 located between the unknown sample portion 6a and the fixed point on the heat conduction plate 6 at which the plate 6 is fixed to the heat reservoir 1. The chromel line 11a co-operates with the material, or constantan, of the heat conduction plate 6, to form a thermocouple 11. A chromel line 12a is welded to a given point 12 located between the reference sample portion 6b and the fixed point on the heat conduction plate 6 at which the plate 6 is fixed to the heat reservoir 1. The chromel lines 11a and 12a are arranged symmetrically. The chromel line 12a co-operates with the material, or constantan, of the heat conduction plate 6, to form a thermocouple 12. A voltage developed between the chromel lines 9a and 11a indicates the temperature difference (ΔT s ) between points 9 and 11 which reflects the electromotive force produced by the chromel-constantan thermocouple. This voltage is applied to an analog-to-digital converter 13, where the voltage is converted into a digital signal. Then, the signal is supplied to the processor 16, where the signal is processed. Similarly, with respect to a temperature difference (ΔT r ) between the points 10 and 12, a voltage generated between the chromel lines 10a and 12a is fed to an analog-to-digital converter 14, where the voltage is converted into a digital form. The signal from the converter is supplied to the processor 16, where the signal is processed. A voltage developed between the chromel line 9a and the alumel line 9b indicates the temperature at the point 9 located at the underside of the unknown sample portion, the temperature reflecting the electromotive force produced by the chromel-alumel thermocouple. This voltage is converted into digital form by an analog-to-digital converter 15 and then sent as a signal T s indicative of the temperature of the unknown sample 8 to the processor 16, where the signal is processed. The processor 16 sends to the furnace temperature control circuit 3 a function of a program about a desired temperature to which the temperature of the heat reservoir 1 should be controlled. In addition, the processor 16 sends the signal applied from the A/D converters 13, 14 and 15 either directly to a recorder means such as a plotter 17 or via a mathematical processing means which mathematically processes the signals in a given manner. In the operation of the present instrument, the operator first enters a temperature rise speed B (°C/min) increasing linearly with respect to time, an AC modulation frequency f (Hz), and an AC modulation amplitude A (°C) into the processor 16. The processor 16 which is triggered by the operator's instruction for starting a measurement produces a temperature program function T p (t) with respect to time t (s) to the furnace temperature control circuit 3, the function T p taking the form: T p (t) = Th (0) + B/60 · t - A · sin (2π · f · t) where Th(0) is the temperature of the heat reservoir 1 when the measurement is initiated. The furnace temperature control circuit 3 supplies an output voltage to the heater 4, the output voltage being PID controlled according to the difference between T p and Th. Thus, the temperature Th of the heat reservoir 1 is maintained coincident with T p . As a result, the profile of the temperature of the heat reservoir 1 is substantially identical with the temperature program function T p (t) specified by the operator. At this time, heat is conducted to the unknown sample portion 6a and to the reference sample portion 6b from the heat reservor 1 via the heat conduction plate 6 according to changes in the temperature of the heat reservoir 1 according to the equation of heat conduction. The amount of heat supplied reflects the nature of the unknown sample. A heat flow - q s (mW) indicating the amount of heat supplied to the unknown sample per second is obtained by dividing the temperature difference between two points along the heat flow path by the heat resistance between the two points according to the thermal Ohm's law. Therefore, the heat flow is derived by dividing the temperature difference signal ΔT s (°C) by the heat resistance value R (mW/°C) between the points 9 and 11 inside the heat conduction plate 6. That is, q s (t) = ΔT s (t) / R If the heat flow the symmetrical reference sample is given by - q r (mW), then it can be expressed in the same way as the heat flow to the unknown sample, i.e., q r (t) = ΔT r (t) / R If the operator sets the AC modulation amplitude A to 0, ordinary DSC data is obtained by sending a differential heat flow signal q s - q r from the processor 16 to the plotter 17 and making a record of this signal with respect to the unknown sample temperature T s . On the other hand, where A ≠ 0, each of the signals T s , q s , and q r , takes a form of its average low-frequency signal component on which a signal component having periodicity of frequency f is superimposed. In this case, signals equivalent to ordinary DSC signals can be obtained by using, instead of the signals T s , q s , and q r , their average values "T s ", "q s ", and "q r " taken over their respective one periods (1/f) (i.e., the average output value of values taken during two half periods, respectively, before and after a certain temperature) and plotting differential heat flow signal "q s " - "q r " against "T s ". This "q s " - "q r " signal is produced as a total heat flow component signal from the processor 16 to the plotter 17. The processor 16 finds the amplitudes of the AC components of the signals T s , q s , and q r by the following discrete Fourier transform method. where amp ( ) indicates the AC amplitude of the signal inside the parentheses, | | indicates the absolute value of the value inside, exp ( ) indicates a function expressing the index of the value included in the parentheses, i is the imaginary unit (-1) ½ , and π indicates the ratio of circumference of a circle to its diameter. By using a calculational method similar to the method used in an AC calorimeter, the difference ΔC p (mJ/°C) in AC heat capacity between the unknown sample and the reference sample is found from the AC amplitudes of the signals as follows. ΔCp = Amp(qs) - Amp(qr) 2π f·Amp(Ts) Especially, where the operator performs a measurement in such a way that the container for the reference sample is hollow, the above ΔC p indicates the AC heat capacity of the unknown sample itself. As is well known in the field of AC calorimeters, the AC heat capacity of an unknown sample does not have a latent heat associated with a transistion caused by the unknown sample. The above ΔC p signal is also produced to the plotter 17 from the processor 16. The above differential heat capacity ΔC p can be transformed into the dimension of a heat flow which can be compared with the above-described total heat flow component signal, by multiplying the ΔC p by the average temperature rise rate d"T s "/dt of the unknown sample. That is, the heat capacity component (C p component) is defined by the following equation: Cp component (mw) = -ΔCp(mJ/°C) x dTs dt (°C/s) The heat capacity component obtained in this way is not affected by the latent heat produced by a transition or reaction produced by the unknown sample and, therefore, this component acts to give the baseline when the latent heat is found from the DSC signal. This component is calculated by the processor 16 and sent to the plotter 17. The difference between the above-described total heat flow component signal "q s " - "q r " and the above heat capacity component reflects only the latent heat component. This is defined as the kinetic component signal according to the following equation: kinetic component (mW) = total heat flow component (mW) - total heat capacity component (mW) The kinetic component obtained in this way is also supplied to the plotter 17 from the processor 16. Various signals including the total heat flow component signal, the heat capacity component signal, and the kinetic component signal delivered from the processor 16 as described above are recorded on the plotter 17 with respect to either the average temperature "T s " of the unknown sample, taken over one period, or time. In the present example, thermocouples are used in measuring the temperature differences ΔT s and ΔT r . Commercially available thermomodules and platinum resistors can also be employed. Of course, if a refrigerant such as liquid nitrogen, vaporised refrigerant, or other cooling means is used in conjunction with the heater 4, then the response of the control over the temperature of the heat reservoir is effectively improved. In order to investigate the thermal property of the unknown sample 8, the temperature difference ΔT s between the thermocouple junction 9 on the side of the unknown sample 8 and the thermocouple junction 11 with the heat conduction plate 6 is found while measuring the temperature difference ΔT r between the thermocouple junction 10 on the reference sample portion 6b and the thermocouple junction 12 on the heat conduction plate 6. The difference between these differences ΔT r and ΔT s is found. Thus, the heat capacity and the latent heat of the unknown sample 8 are determined. If the temperature elevation conditions and the reference sample portion 6b remain the same, then the change in ΔT r with respect to time or temperature is maintained constant. Consequently, the above-described measurement object can be accomplished simply by measuring the temperature difference ΔT s . As described thus far, in the present invention, a heat flux type DSC is so improved that a heat flow on the side of an unknown sample and a heat flow on the side of a reference sample can be measured independently and that the temperature of a heat reservoir can be controlled according to a ramp function modulated with an alternating sinusoidal wave. In consequence, DSC measurements can be performed. Additionally, the AC heat capacity of the unknown sample can be measured with high accuracy. Also, only information about the heat capacity can be extracted from a DSC signal which inevitably includes information about the latent heat, as well as the information about the heat capacity. Hence, the baseline of the DSC signal becomes apparent. The latent heat of the unknown sample can be measured accurately. Further, with respect to a complex DSC thermogram, the instrument itself judges whether a change in the DSC signal is caused by a change in the heat capacity of the unknown sample or by a latent heat. Therefore, when data is interpreted, the possibility of human errors is reduced drastically. The aforegoing description has been given by way of example only and it will be appreciated by a person skilled in the art that modifications can be made without departing from the scope of the present invention.

Claims: A thermal analysis instrument comprising: a heat reservoir (1) consisting of a good thermal conductor; a constant rate temperature-varying means (2, 3, 4) for varying temperature of said heat reservoir at a constant rate; an alternating temperature-varying means (16) for varying the temperature of said heat reservoir according to a periodical function having given frequency and amplitude; the temperature of said heat reservoir being varied according to a ramp function which is AC modulated by said constant rate temperature-varying means and by said alternating temperature-varying means, characterised by a heat resistor (6) for connecting said heat reservoir with an unknown sample position and with a reference sample position symmetrically and forming heat flow paths; a sample temperature-measuring means for measuring temperature at a point that is located on said heat resistor and close to the unknown sample; characterized in that it comprises: a first temperature difference-measuring means (9, 11, 13, 15) for measuring a heat flow in one of the heat flow paths between a given point (9) close to the unknown sample position and a fixed point (11) as a temperature difference, said fixed point being located between the heat reservoir and the unknown sample; a second temperature difference-measuring means (10, 12, 14) for measuring a heat flow in the other of the heat flow paths between a given point (10) close to the reference sample position and a second fixed point (12) as a temperature difference, said second fixed point being located between the heat reservoir and the reference sample, said first and second temperature difference-measuring means being formed symmetrically; and The thermal analysis instrument of claim 1, characterized in that said periodical function is a sinusoidal wave. The thermal analysis instrument of claim 1 or 2, characterized in that a difference between the output from said first temperature difference-measuring means and the output from said second temperature difference-measuring means is delivered as a signal used for differential scanning calorimetry. The thermal analysis instrument of claim 1, 2 or 3, characterized in that output signals from said first temperature difference-measuring means, from said second temperature difference-measuring means, and from said sample temperature-measuring means can be passed through filters, whereby each signal is divided into an AC amplitude corresponding to a frequency of said periodical function and a low frequency component independent of said frequency. The thermal analysis instrument of claim 4, characterized in that a difference between the low frequency component from said first temperature difference-measuring means and the low frequency component from said second temperature difference measuring means is delivered as a total heat flow component signal. The thermal analysis instrument of claim 4, characterized in that a heat capacity of the unknown sample is found according to a ratio of a difference between AC amplitude of the output from said first temperature difference-measuring means and AC amplitude of the output from said second temperature difference-measuring means to AC amplitude of the output from said sample temperature-measuring means. The thermal analysis instrument of claim 5, characterized in that a heat capacity of the unknown sample is found according to a ratio of a difference between AC amplitude of the output from said first temperature difference-measuring means and AC amplitude of the output from said second temperature difference-measuring means to AC amplitude of the output from said sample temperature-measuring means. The thermal analysis instrument of claim 7, characterized in that the heat capacity of the unknown sample is found according to the ratio between said AC amplitudes is multiplied by an average rate of change of the low-frequency component of the output signal from said sample temperature-measuring means, whereby a signal is transformed into a dimension of heat flow and is delivered as a signal indicative of a component of the heat capacity. The thermal analysis instrument of claim 8, characterized in that a difference between said total heat flow component signal and said signal indicative of a component of the heat capacity is delivered as a kinetic component signal.

Inventors: NAKAMURA NOBUTAKA, TERAMOTO YOSHIHIKO, NAKAMURA, NOBUTAKA, TERAMOTO, YOSHIHIKO
Applicants: SEIKO INSTR INC, SEIKO INSTRUMENTS INC.
Application year: 1994
Main classification: G01N25
IPC codes: G01N25